Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 16
... ΦΩ 2 | f | 2 1 ( 27 ) 2 / d28 [ db exp ( ið · b ) y ( b ) f d'b ' exp ( -id.b ′ ) y * ( b ′ ) Remark : do ΦΩ = 15 ( 8 ) 1 | 2 , = = J do de sin o do | f2≈ For small we have : hence d28d8 8 do k20 do do , σel = [ ď2b | v ( b ) | 2 . Now ...
... ΦΩ 2 | f | 2 1 ( 27 ) 2 / d28 [ db exp ( ið · b ) y ( b ) f d'b ' exp ( -id.b ′ ) y * ( b ′ ) Remark : do ΦΩ = 15 ( 8 ) 1 | 2 , = = J do de sin o do | f2≈ For small we have : hence d28d8 8 do k20 do do , σel = [ ď2b | v ( b ) | 2 . Now ...
Page 19
... ΦΩ = | Im M2 + Re M 2 . The amplitude ( 3.6 ) has some simple properties which show that the Coulomb interaction may help us in learning about the real part of the strong interaction phase shift , ( b ) ( which is , as a rule , not well ...
... ΦΩ = | Im M2 + Re M 2 . The amplitude ( 3.6 ) has some simple properties which show that the Coulomb interaction may help us in learning about the real part of the strong interaction phase shift , ( b ) ( which is , as a rule , not well ...
Page 22
... ΦΩ = do sc ΦΩ ΦΩ doel = d2b d'b ' exp [ i △ · ( b − b ' ) ] • 2π 2 × [ ( % | г + ( b ) гT ( b ) | Yo ) — ( Yo | г + ( b ) | Yo ) ( Yo | г ( b ) | Yo ) ] . It is an interesting fact that while doe / d is very strongly influenced by ...
... ΦΩ = do sc ΦΩ ΦΩ doel = d2b d'b ' exp [ i △ · ( b − b ' ) ] • 2π 2 × [ ( % | г + ( b ) гT ( b ) | Yo ) — ( Yo | г + ( b ) | Yo ) ( Yo | г ( b ) | Yo ) ] . It is an interesting fact that while doe / d is very strongly influenced by ...
Page 26
... ΦΩ = 1 3 m , m | ( m | M ( △ , s ) | m ′ ) | 2 with ik M ( A , s ) = d2b exp ( i △ · b ) { 1— exp [ ix , ( b − 1⁄2s ) + ixn ( b + 28 ) ] } , 2π which operator , in this approximation , does not depend on spins . So , if not for the ...
... ΦΩ = 1 3 m , m | ( m | M ( △ , s ) | m ′ ) | 2 with ik M ( A , s ) = d2b exp ( i △ · b ) { 1— exp [ ix , ( b − 1⁄2s ) + ixn ( b + 28 ) ] } , 2π which operator , in this approximation , does not depend on spins . So , if not for the ...
Page 44
... ΦΩ 0 where ny is the ratio of the real to the imaginary part of M ( y - V ) . So , finally , the relation which can be tested is as follows : Σ Αν πα П OT ( Y , hadron ) = ky V γν ( 1 + n2 ) -1/2 ) dov | 1 ) TH 1/2 ( 4.8 ) By measuring ...
... ΦΩ 0 where ny is the ratio of the real to the imaginary part of M ( y - V ) . So , finally , the relation which can be tested is as follows : Σ Αν πα П OT ( Y , hadron ) = ky V γν ( 1 + n2 ) -1/2 ) dov | 1 ) TH 1/2 ( 4.8 ) By measuring ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db bJo db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function Απ γν ΦΩ